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EP 0 472 717 B1 |
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EUROPEAN PATENT SPECIFICATION |
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Mention of the grant of the patent: |
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04.06.1997 Bulletin 1997/23 |
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Date of filing: 14.03.1991 |
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International application number: |
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PCT/US9101/702 |
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International publication number: |
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WO 9114/285 (19.09.1991 Gazette 1991/22) |
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SEMICONDUCTOR CHIP GYROSCOPIC TRANSDUCER
HALBLEITERCHIP MIT GYROSKOPISCHEM WANDLER
TRANSDUCTEUR GYROSCOPIQUE A MICROPLAQUETTE SEMI-CONDUCTRICE
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Designated Contracting States: |
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AT BE CH DE DK ES FR GB GR IT LI LU NL SE |
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Priority: |
14.03.1990 US 493327
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Date of publication of application: |
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04.03.1992 Bulletin 1992/10 |
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Proprietor: THE CHARLES STARK DRAPER LABORATORY, INC. |
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Cambridge, MA 02139-3563 (US) |
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Inventor: |
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- GREIFF, Paul
Wayland, MA 01778 (US)
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Representative: Reinhard - Skuhra - Weise & Partner |
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Postfach 44 01 51 80750 München 80750 München (DE) |
| (56) |
References cited: :
EP-A- 0 443 280 US-A- 4 483 194 US-A- 4 628 283 US-A- 4 674 319 US-A- 4 699 006 US-A- 4 736 629
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US-A- 4 342 227 US-A- 4 598 585 US-A- 4 670 092 US-A- 4 680 606 US-A- 4 705 659
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- Sensors and Actuators - A21-A23 (1990), Elsevier, NL, pp.273-277; B.Boxenhorn et al.:
"Monolithic Silicon Accelerometer"
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| Note: Within nine months from the publication of the mention of the grant of the European
patent, any person may give notice to the European Patent Office of opposition to
the European patent
granted. Notice of opposition shall be filed in a written reasoned statement. It shall
not be deemed to
have been filed until the opposition fee has been paid. (Art. 99(1) European Patent
Convention).
|
TECHNICAL FIELD
[0001] This invention relates to gyroscopic transducers and, in particular to gyroscopic
transducers manufactured using semiconductor fabrication processes.
BACKGROUND ART
[0002] Semiconductor fabrication techniques are in use to produce micromechanical structures
from silicon wafers. Such micromechanical structures have the potential of mass production
at a very low cost.
[0003] Illustrative of this particular technology is U.S. Patent No. 4,598,585 to Boxenhorn,
which discloses a planar micromechanical vibratory gyroscope adapted for small geometry
configurations which may be constructed using semiconductor fabrication mass production
techniques.
[0004] Further advances in micromechanical gyroscopic transducer technology are described
in Applicant's co-pending U.S. Patent Application Serial No. 07/143,515, filed January
13, 1988, entitled METHOD AND APPARATUS FOR SEMICONDUCTOR CHIP TRANSDUCER and U.S.
Application Serial No. 07/143,515, Filed January 13, 1988, entitled METHOD AND APPARATUS
FOR SEMICONDUCTOR CHIP TRANSDUCER.
[0005] Other advances in micromechanical gyroscopic technology are described in Applicant's
pending U.S. Patent Application US-A-5 216 490 entitled BRIDGE ELECTRODES.
[0006] The infancy of monolithic micromechanical semiconductor gyroscopic transduction technology
assures that significant advances will continue to be made with respect to implementation
and application of the technology. As structures are implemented having increased
sensitivity and accuracy, problem areas are identified and solutions defined. Presently,
shortcomings with respect to "rippling" of an oxide support frame from which an outer
flexure extends connecting a resonating structure thereto are observable. "Buckling"
of inner flexures, results in undesirable large variations in a critical resonant
frequency of a suspended gyroscopic element. Furthermore, surface bridge electrodes
used for sensing and for rebalancing of a certain axis of a resonating structure have
large capacitances to the substrate limiting effectiveness as signal pickoffs.
[0007] Further document US-A-4 699 006 discloses further details of such monolithic semiconductor
designs in accelerometers and gyroscopes. This document in particular details a gyroscope
which basically comprises a semiconductor mass with a recess, above which is positioned
a transducer element with first and second gimballed plates integrally linked to the
mass, respectively the first plate via flexing links. The second plate bears a balanced
mass, and sets of electrodes are provided in, i.e. integral to the semiconductor mass.
[0008] Prior art document Sensors and Actuators, A21-A23, Feb'90, Elsevier Sequoia (NL),
pp 273-277; Boxenhorn et al.: "Monolithic Silicon Accelerometer" describes further
developments in design and manufacture of monolithic silicon micromechanical accelerometers.
This document in particular suggests the use of bridge electrodes spanning the gimbal
plate of the accelerometer, in order to produce more symmetrical torquing and better
linearity.
SUMMARY OF THE INVENTION
[0009] The above problems are solved by a gyroscope having the features of claim 1.
BRIEF DESCRIPTION OF THE DRAWING
[0010] The invention will be more fully understood from the following detailed description
of illustrative embodiments taken in conjunction with the accompanying drawing in
which:
Fig. 1 is a perspective view partially cut away of a semiconductor chip gyroscopic
transducer according to the invention;
Fig. 2 is an expanded view of a semiconductor chip gyroscopic transducer flexure/frame
junction with a footing according to the invention;
Fig. 2A is an expanded side view of a P-type footing disposed at the flexure/frame
junction of Fig. 2;
Fig. 3 is a conceptual view of a semiconductor chip gyroscopic transducer having a
strain relief and torsional stiffness system and footings according to the invention;
Fig. 3A is a side sectional view of flexure grooves according to the invention, formed
by plasma etching
Fig. 3B is a side sectional view of flexure grooves according to the invention, formed
by anisotropic etching;
Fig. 4 is a cross-section view of the semiconductor chip gyroscopic transducer of
Fig. 1 taken along a line Y-Y;
Fig. 4A is a top view of an electrically isolated bridge electrode landing;
Fig. 4B is a side section view of the isolated landing of Fig. 4A;
Fig. 4C is a top, diagrammatic view of a micromechanical gyroscopic transducer having
signal pickoff by inner bridge electrodes with electrically isolated landings;
Fig. 5 is an alternative embodiment of a semiconductor chip gyroscopic transducer
having four buried electrodes and two bridge electrodes according to the invention;
Fig. 6A is a side section and perspective view of a micromechanical gyroscopic transducer
having an on-chip JFET buffer for amplifying a signal picked off of a flexure;
Fig. 6B is a schematic diagram of a micromechanical gyroscopic transducer including
the on-chip JFET buffer amplifier of Fig. 6A;
Fig. 6C is a schematic diagram of electronic circuitry for the gyroscopic transducer
of Fig. 4C having bridge electrode signal pickoff; and
Fig. 6D is a side section and perspective view of a micromechanical gyroscopic transducer
having on-chip JFET buffer circuitry in proximity to pickoff bridge electrodes.
DETAILED DESCRIPTION OF THE INVENTION
[0011] A micromechanical gyroscopic transducer 10, as viewed in Fig. 1, is formed from a
mass of N-type silicon 12. Mass 12 is preferably an N-type epitaxially grown layer
13 on a base of monocrystalline N-type silicon 15. Selective etching of the silicon
12 as described in the above-referenced applications yields a void 14 within a silicon
frame 16. A transducer element 18, which has been doped P-type and is freed from silicon
mass 12 as a result of selective etching is suspended above the void 14. The transducer
element 18, comprising outer and inner portions 32 and 34 respectively, is supported
by flexible links or flexures 20 and 22, similarly freed by selective etching, which
provide first flexible linkage means coupling the portion 32 of transducer element
18 to the silicon frame 16. Flexures 20 and 22 each have first ends 24 and 26 respectively,
extending from the silicon frame 16. Second ends 28 and 30 of flexures 20 and 22 respectively,
connect with the first portion or gimbal plate 32 of the transducer element 18. First
gimbal plate 32 flexibly supported by flexures 20 and 22 is capable of limited rotation
about an X-axis extending through flexures 20 and 22.
[0012] Interior to gimbal plate 32 of transducer element 18 is the second portion, or a
second gimbal plate 34. A second set of flexures 36 and 38 provide a second flexible
linkage means for coupling the second gimbal plate 34 to the first gimbal plate 32.
Second flexures 36,38 have first ends 40,42 and second ends 44,46, respectively. The
first ends 40,42 of flexures 36,38 are connected to first gimbal plate 32. The second
ends 44,46 are connected to second gimbal plate 34. Second gimbal plate 34 is capable
of limited rotation about a Y-axis, orthogonal to the X-axis, extending through the
first ends 40,42 and second ends 44,46 of the flexures 36,38 respectively. Second
gimbal plate 34 supports a centrally located mass 48 which is substantially balanced
between top and bottom of the second gimbal plate 34. Substantially balanced mass
48 is formed on second gimbal plate 34 by selectively etching a trough therein. The
process, discussed in significant detail in above-referenced U.S. Patent Application
Serial No. 143,515, includes provision of a deep pit, through the surface of silicon
mass 12 where mass 48 is to be located, prior to etch resistant doping of the plate
34. After etching, the pit remains and may be filled with single crystal or polysilicon
followed by a solid electroplating on a layer of titanium tungsten (TiW) covered with
a layer of gold (Au) deposited via vacuum deposition. A mass of gold may alternatively
be electroplated into the pit on the layer of vacuum deposited gold. A Z-axis is defined
by the central location of the topside and bottomside of the substantially balanced
mass 48. The process of metal plating on silicon is discussed below.
[0013] In the illustrative embodiment of Fig. 1, the micromechanical gyroscopic transducer
10 has four integral or buried electrodes 50,52,54,56 extending beneath the first
gimbal plate 32 substantially parallel to the X-axis. The buried electrodes 50,52,54,56
are typically P+ doped semiconductor material formed in base layer 15 prior to the
growth of epitaxial layer 13. With the typically N-type silicon mass these form P-N
junctions. Typically, two of the electrodes are used for torquing the transducer element
18 and two are used for sensing and vibration angle amplitude control. Buried electrode
functionality is facilitated by electrical connection through a deep P+ diffusion
to the buried electrodes which are in turn surface metallized and connected to contacts
51,53,61,63 on frame 16 which are in turn electrically connected to associated on-
or off-chip drive and sense electronics 55 on signal bus 57 that cause controlled
amplitude vibration of plate 32 as discussed below.
[0014] Additionally, the micromechanical gyroscopic transducer 10 has four surface bridging
electrodes 58,60,62 and 64 which span the transducer element 18 and are bonded to
silicon frame 16 at respective electrode landings 66,68,70,72, 74,76,78 and 80. The
bridge electrodes 58,60,62,64 reside above the second gimbal plate 34, two each on
either side of substantially balanced mass 48, parallel to the Y-axis defined by first
and second ends of flexures 36,38 for torquing and sensing position of the plate 34.
For this purpose, they are connected to signal bus 57 and electronics 55. Bridge electrodes
are fabricated using metal plating technology discussed in the referenced application.
[0015] Functionally, the second gimbal plate 34 with substantially balanced mass 48 supported
by flexures 44,46 is the gyro sensing element. First gimbal plate 32 is a driven member
which is caused to vibrate at a fixed frequency and angular amplitude about the X-axis.
The fixed frequency of vibration with which the first gimbal plate 32 is driven is
the resonant frequency of the second gimbal plate 34 with substantially balanced mass
48. Vibration of the first gimbal plate 32 is induced by applying appropriate alternating
DC voltages to the outer buried electrodes 50,56, in order to produce an electrostatic
torque. The inner buried electrodes 52,54 sense first gimbal plate 32 vibration angle
amplitude. Electronics 55 provides feedback control over the torque to insure a fixed
amplitude. The torque electrodes are preferably buried for stability. The resulting
dynamical system is sensitive to rotation of the structure about a Z-axis orthogonal
to the X and Y axes and passing through the balanced mass 48. When rotation of the
system about the Z-axis occurs, second gimbal plate 34 with substantially balanced
mass 48 oscillates at its resonant frequency at an amplitude proportional to the rate
of rotation applied.
[0016] Surface bridge electrodes 58,60,62,64 spanning transducer element 18 in proximity
to second gimbal plate 34 are used for sensing and for rebalance of the second gimbal
plate 34 with substantially balanced mass 48, nulling its tendency to vibrate. Because
the gyro described hereinbefore in an open loop condition is very sensitive to parameter
variations such as small changes in the resonant frequency of second gimbal plate
34 or small changes in the angle of vibration, it is a practical necessity to operate
the gyro in a closed loop condition to minimize this sensitivity. Closed loop operation
requires that the gyro be incorporated into a rebalance loop that maintains second
gimbal plate 34 at null by torquing the second gimbal plate 34 electrostatically.
By torquing second gimbal plate 34 null the gyro system can tolerate variations in
vibration frequency. Closed loop operation enables the drive vibration angle amplitude
of first gimbal plate 32 to be increased without cross-coupling interactions with
the second gimbal plate 34, since second gimbal plate 34 is maintained near null by
closed loop rebalancing.
[0017] Closed loop rebalancing is facilitated by two quadrature servo-loops in electronics
55 operating in conjunction. The servo-control electronics, as shown in the referenced
application, will rebalance second gimbal plate 34 so that the effect on nonorthogonality
of the gimbals and the unbalance of the second gimbal plate 34 will be minimized.
The output of the control electronics 55 is a voltage proportional to the torque required
to rebalance the second gimbal plate 34 against gyroscopic torques. A third servo-controlled
loop is required to maintain vibration drive angle of first gimbal plate 32 at a fixed
value. The third servo-control loop is similar to the control loops of second gimbal
plate 34 but allows a much lower bandwidth.
[0018] The desirability of surface bridge electrodes as opposed to an increased number of
integral or buried electrodes, results from a large voltage dependent parasitic capacitance
to the semiconductor mass 12 inherent in such buried electrodes. Furthermore, buried
electrodes exhibit a small leakage current and are limited with respect to the voltage
which can be applied, that being the reverse breakdown voltage of a P-N junction,
typically about 40 volts. Buried electrode utility is also limited in a micromechanical
gyroscopic transducer application since although they can be disposed in a manner
parallel to an X-axis of rotation of the first gimbal plate they cannot concurrently
be disposed in a manner perpendicular to that same axis of rotation (or parallel to
a Y-axis of rotation of the second gimbal plate). Because surface bridge electrodes
can be disposed perpendicular to buried electrodes, the surface bridge electrodes
can be aligned in proximity and parallel to the axis of rotation of second gimbal
plate 34 while buried electrodes are aligned in proximity and parallel to the axis
of rotation of first gimbal plate 32. A single pair of bridge electrodes can replace
the double pair 58,60,62 and 64 by using separate frequencies for sensing and rebalance
torquing. Furthermore, a pair of surface bridge electrodes may be used as differential
signal pickoffs as discussed hereinafter.
[0019] In the selective etching of void 14, wherein silicon frame 16, the double gimbal
plates 32,34 and double flexible linkage system are left intact, an undercutting of
silicon dioxide surface portions adjacent flexures 20 and 22 leaves an unsupported
lip 82 which is subject to rippling (Fig. 2). The geometric variations induced by
rippling along the lip 82 causes a variation in twist on flexures 20,22 supporting
transducer element 18 in silicon frame 16. The resultant twisting forces exerted on
the flexures 20,22, caused by the rippling, adversely impact the vibratory characteristics
and angular bias of first gimbal plate 32 which consequently affects the gyroscopic
sensitivity of second gimbal plate 34. The detrimental effect of the rippling of the
silicon dioxide lip 82 which is typically 0.6 micron in thickness at the undercut,
according to the invention, is prevented by employing a 3 micron P-type diffusion
or footing 84 at the junction of flexures 20,22 and silicon frame 16. The disposition
of footing 84 is best viewed in Fig. 2A. It can be seen that N-type silicon frame
16 has disposed therein P-type footing 84 at the junction of silicon frame 16 and
flexures 20 and 22 which prevents undercutting to either side of the flexures 20,22
by the selective etching of void 14. P-type footing 84 acts as a buffer between rippled
portions 82 precluding the twisting which otherwise results, while maintaining P-N
junction isolation of the double gimbal double flexure transducer from silicon frame
16.
[0020] Referring now to Fig. 3, a double flexure double gimbal plate micromechanical gyroscopic
transducer is provided, in combination, with a strain relief and torsional stiffness
system. This is provided by grooved flexures and strain relieving slots defining tension
relief beams at the junction of the flexures and outer gimbal plate 32.
[0021] As shown there, gimbal plate 32 has disposed therein four slots 86,88,90 and 92,
which form stress relief beams 94,96,98 and 100, respectively. Slots 86 and 90 are
disposed in proximity to the inner ends of flexures 20 and 22 such that the tension
relief beams 94 and 98 are formed at the point where the flexures 20,22 join the plate
32. Slots 88 and 92 are placed where flexures 36 and 38 join plate 32 and form beams
96 and 100.
[0022] The outer gimbal 32 is in tension because its etch resistance results from boron
doping which reduces the lattice spacing with respect to the surrounding N-type doped
mass 12. The result is that the undercut structure tries to shrink but is restrained
by the larger stiffer mass 12 and this puts gimbal plate 32 in tension. In the axis
through flexures 36,38 the structure is free to shrink. Since the gimbal 32 is thicker
than the flexures 36,38 it must be more heavily doped and therefore shrinks at a higher
rate putting flexures 36,38 in compression. Beams 94,96,98 and 100 are trimmable.
The slot that creates the beam which alleviates the tension forces on the plate 32
also affects the resonant frequency of gimbal plate 32. By trimming the slot and beam
sizes the resonant frequency can be controlled. Trimming beams 96,100, provides compression
relief as discussed above.
[0023] Grooves 102 and 104 are formed in flexures 36 and 38 respectively. While stress relieving
beams 96 and 100 impact the torsional dynamics of the second flexible linkage means,
grooves 102 and 104 provide a three-dimensional beam structure that is relatively
soft in the desired torsional mode yet is substantially stiffer. This reduces unwanted
buckling or bending of flexures 36 and 38. The same kind of grooves may be provided
in flexures 20 and 22 with the same result, although they are not shown.
[0024] Figs. 3A and 3B illustrate the construction of such a groove. Pits 102,104 are formed
by a plasma or other etching process, as known in the art, prior to the P-type diffusion
that defines the flexures. The diffusion thus takes the form of a groove or channel,
providing box beam stiffening.
[0025] Referring now to Fig. 4, there is shown a cross-sectional view of the micromechanical
gyroscopic transducer, according to the invention. A bridge electrode 64 is shown
and is constructed in a manner described in U.S. Patent Application Serial No. 372,653
entitled BRIDGE ELECTRODES. Another bridge electrode 58 is located behind electrode
64 and therewith span the transducer element 18 above the second gimbal plate 34,
a few microns therefrom.
[0026] Each bridge electrode has opposite landings or terminations represented by landings
106,108 illustrated in Figs. 4, 4A, 4B and 4C, disposed on the silicon frame 16. The
electrode landings are formed over metallization layer 110. An oxide layer 113- provides
DC electrical isolation but capacitance to substrate is still large. In some cases
(i.e. where the bridge electrodes are used at high impedance for signal pickoff instead
of excitation from a low impedance source) this capacitance adversely affects the
signal.
[0027] The construction illustrated in Figs. 4A and 4B provides a driven shield to effectively
neutralize this capacitance. As shown also in Fig. 4C electrical isolation regions
111 and 111a are provided under the landings of the signal pickoff bridges 64 and
58. In the discussion to follow it is understood that both regions 111, on both sides
of the bridge, are treated the same electrically. This is true of regions 111a as
well. Regions 111 and 111a are DC isolated by the surrounding P regions 112,114. By
circuitry described below and illustrated in Fig. 6C, the region 111 is driven at
the same (or nearly the same) potential as electrode landing 106 and the capacitance
between them is thus electrically neutralized, maximizing the signal-to-noise ratio
at the point of pickoff.
[0028] An alternative electrode arrangement for a micromechanical gyroscopic transducer,
according to the invention, is illustrated in Fig. 5. In this embodiment four buried
electrodes are configured in combination with two surface bridge electrodes one each
replacing a pair 58/60 and 62/64 of Fig. 1, to effect the micromechanical gyroscopic
transduction function as described hereinbefore.
[0029] Outer buried electrodes 118,120 are disposed below outer gimbal plate 32 parallel
to the axis formed by the flexures 20,22 and serve as torquing electrodes providing
the function of driving outer gimbal plate 32 at one frequency, sensing the displacement
at a second frequency and controlling the first frequency drive to achieve a controlled
vibration as described in the referenced application.
[0030] Inner buried electrodes 122,124, are disposed between buried electrodes 118,120 and
loop beneath opposite ends of plate 34 from opposite ends of transducer element 18.
Inner buried electrodes 112,124 provide the function of rebalance torquing, with a
drive voltage, typically 1.0 mV, which rebalances or drives to null inner gimbal plate
34 with mass 48. Inner buried electrodes 122,124 have cutouts 126,128 around the region
of flexures 20,22.
[0031] In this embodiment, two surface bridge electrodes, not shown, are configured as discussed
hereinbefore with respect to the four bridge electrodes of Fig. 1. However, whereas
four bridge electrodes were configured in proximity to inner gimbal plate 34, two
on either side of balanced mass 48, parallel to the Y-axis defined by first and second
ends of flexures 36,38, in the embodiment of Fig. 5, only one bridge electrode is
configured on either side of balanced mass 48, parallel to the Y-axis and in proximity
to inner gimbal plate 34. The two bridge electrodes are used to sense inner gimbal
plate 34 motion, while an excitation frequency is applied through flexures to the
inner gimbal plate 34. The bridge electrode may be located to provide vertical symmetry
with respect to the rebalance torquing buried electrodes 122,124.
[0032] Shown in Fig. 6A is electrical circuitry for on-chip signal processing to limit the
effect of parasitic capacitance in long signal paths in an embodiment wherein an excitation
frequency is applied to inner gimbal plate 34 through bridge or buried electrodes
and a signal indicating inner gimbal 34 motion is sensed at a flexure node 200. An
electrical equivalent circuit diagram, illustrated in Fig. 6B, of the micromechanical
gyroscopic transducer capacitances includes capacitances C
1-C
n and Cp wherein C
1-C
n represent the variable capacitances resulting from the distance of the inner gimbal
plate 34 relative to n excited buried and bridge electrodes. The resulting signal
at the gimbal plate 34 is sensed through flexures and outer gimbal plate 32 to frame
16. A parasitic capacitance Cp between the structure 18 and the semiconductor mass
12 acts as a shunt and is large enough to reduce the signal to noise ratio particularly
if it includes any length of signal path prior to impedance buffering. For this purpose
the gimbal signal is buffer amplified by an on-chip JFET which minimizes the effect
of shunt capacitance from long lead lengths by reducing the impedance of the signal
for application to off-chip electronics 55 as described in the above-referenced application
to provide the signals necessary to electronically torque the instrument and derive
rate outputs.
[0033] As illustrated in Fig. 6B the signal from the inner gimbal 34 is present at output
node 200 which is connected to the gate of a high input impedance JFET Q
1 which is fabricated on-chip and proximate to the signal source as an impedance buffering
preamplifier to overcome the effects of parasitic capacitance. Transistor Q
2 is fabricated along with Q
1 as a matched pair. In connection with amplifier A
1 (on- or off-chip), it serves to bias the gate of Q
1 at a virtual ground. This provides a stable reference for the torque electrodes shown
as C
n. Electronics 55 provides the drive signals for capacitors C
1 through C
n, the biases for R
1 and the drains of Q
1 and Q
2. Amplifier A
1 is typically a unity voltage gain high gain amplifier providing feedback to an on-chip
RC combination R
1 and C
10 which provides signal stabilization. The output of operational amplifier A
1 is processed by electronics 55.
[0034] As illustrated in Fig. 6A the on-chip JFET buffer amplifier Q
1 is fabricated on the chip in proximity to a flexure frame junction to ensure minimum
parasitic capacitance and high stability. Furthermore, the RC combination of R
1 and C
10 may also be provided on-chip. R
1 may be fabricated in the megohm range from polysilicon or it may be formed on-chip
as a biased JFET as shown in Fig. 6B. C
10 may be a MOS device fabricated on-chip. The p regions 150 doped to act as sources
and drain (the p channel 152 and the gate 154 being diffused separately) in the on-chip
JFETs may be fabricated as highly doped regions during the boron doping process steps
used to make flexure and gimbal plate etch resistant structures as discussed hereinbefore
or in separate steps. Metalliza- tions 156 and 158 for the source and drain and for
gate 154, respectively required for electrical contact to the on-chip JFET can be
provided during metallization process steps undertaken during the fabrication of the
micromechanical gyroscopic transducer structure as described in the above. Metalization
154 extends to an aperture in layer 160 where it contacts a doped flexure to the outer
gimbal plate.
[0035] An embodiment wherein an excitation frequency is applied to inner gimbal 34, as illustrated
in Fig. 4C, may provide a better signal-to-noise ratio when the signal indicating
inner gimbal 34 motion is sensed differentially by a pair of surface bridge electrodes
58,64. Surface bridge electrodes, as discussed in the referenced application, can
provide lower capacitance than buried electrodes and can be electrically isolated
by driven shields provided at the bridge electrode landings 106 as discussed hereinbefore
with respect to Figs. 4, 4A, 4B and 4C. An electrical model of such a configuration
and an illustration of a JFET buffer preamplifier located proximate to the bridge
electrode landing are shown in Figs. 6C and 6D, respectively.
[0036] Referring to Figs. 6C and 6D, a high frequency approximately 100 kHz signal is inserted
on inner gimbal plate 34 by electronics 55. Bridges 64 and 58 serve as a differential
capacitive pickoff. Areas 110,110a of the bridges have relatively high capacitance
to the electrically isolated regions 111,111a. The differential signals from C
1 and C
2 are fed to the gates of JFETs Q
1 and Q
1a which serve as buffer amplifiers to greatly lower the signal impedance and isolate
it from electrical interference. Transistors Q
2 and Q
2a and external electronics 55 (not shown in Fig. ) form a biasing network for the gates
of Q
1 and Q
1a. Amplifier A
1 is a differential amplifier (either on- or off-chip) which differences and amplifies
the positional signal. Nodes N
1 and N
1a are low impedance reference nodes which track the gate voltage in phase and amplitude
and which may be used to drive regions 111 and 111a thereby effectively neutralizing
the parasitic capacitance from regions 110,110a to 111,111a. The result is a greater
signal-to-noise ratio.
[0037] Although the invention has been shown and described with respect to exemplary embodiments
thereof various other changes, omissions and additions in form and detail thereof
may be made therein without departing from the scope of the invention as defined in
the appended claims.
1. A micromechanical gyroscopic transducer comprising:
a mass (12) of semiconductor material having a void (14) on a top surface extending
downward, said mass of silicon comprising a silicon frame (16);
a transducer element (18) suspended above said void (14), said transducer element
(18) comprising:
first and second flexible linkages (20, 22) integral with said frame material (16)
for coupling said transducer element to said frame (16) at opposite ends, first ends
(24, 26) of said first flexible linkages (20, 22) being connected to said silicon
frame (16);
a first gimbal plate (32) integral with said frame material (16) connected to said
second ends (28, 30) of said first and second flexible linkages (20, 22), said first
gimbal plate (32) being capable of oscillatory motion about an axis through said first
and second flexible linkages (20, 22);
a second gimbal plate (34), interior to said first gimbal plate (32);
third and fourth flexible linkages (36, 38) integral with said frame material (16)
coupling said second gimbal plate (34) to said first gimbal plate (32) on opposite
ends, said third and fourth flexible linkages (36, 38) having first ends (40, 42)
and second ends (44, 46), said first ends of said third and fourth flexible linkages
(36, 38) being connected to said first gimbal plate (32) and said second ends of said
third and fourth flexible linkages (36, 38) being connected to said second gimbal
plate (34), said second gimbal plate (34) being capable of oscillatory motion about
an axis through said third and fourth flexible linkages (36, 38);
a substantially balanced mass (48), central to said second gimbal plate (34), said
substantially balanced mass (48) having a top side and a bottom side defining an axis
therebetween;
first and second sets of electrodes (50, 52, 54, 56) configured within said mass (12)
in a bottom region of said void (14) and integral with said frame material, said first
set of integral electrodes facing said first gimbal plate (32) and said second set
of integral electrodes facing said second gimbal plate (34);
characterized in that
a plurality of bridge electrodes (58, 60, 62, 64) are configured above said transducer
element (18), each of said plurality of bridge electrodes (58, 60, 62, 64) being supported
from said frame (16) at an electrode landing (106, 108) and extending over at least
one of said first (32) and second (34) gimbal plates,
each of said bridge electrodes (58, 60, 62, 64) are supported from said frame on a
region of doped material (111, 112, 114) disposed between and in electrical communication
with said bridge electrodes (58, 60, 62, 64) and said mass material (12)
wherein said region of doped material (111, 112, 114) comprises an intermediate area
(111) isolated by surrounding areas (112, 114), said intermediate area (111) in use
being biased relative to said mass material (12) so as to effectively isolate said
bridge electrodes (58, 60, 62, 64) from said mass material (12).
2. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said mass (12) is monocrystalline silicon (15) and said void (14) is anisotropically
etched therein.
3. The micromechanical gyroscopic transducer of claim 2,
characterized in that
said first and second gimbal plates (32, 34) include etch resistant dopants and are
formed by selective etching of said mass (12).
4. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said flexible linkages (20, 22, 36, 38) include etch resistant dopants and are formed
by selective etching of said mass (12).
5. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said first gimbal plate (32) includes means (94, 96, 98, 100) for relieving stress
adjacent one or more of said flexible linkages (20, 22, 36, 38).
6. The micromechanical gyroscopic transducer of claim 5,
characterized in that
said means for relieving stress comprises a beam (94, 96, 98, 100) created by a slot
(86, 88, 90, 92).
7. The micromechanical gyroscopic transducer of claim 6,
characterized in that
said slot (86, 90) is proximate to said second ends of said first and second flexible
linkages (20, 22).
8. The micromechanical gyroscopic transducer of claim 6,
characterized in that
said slot (86, 90) is orthogonally disposed with respect to said axis of said first
and second flexible linkages (20, 22).
9. The micromechanical gyroscope transducer of claim 6,
characterized in that
said slot (88, 92) is proximate to said first ends of said third and fourth flexible
linkages (36, 38).
10. The micromechanical gyroscopic transducer of claim 6,
characterized in that
said slot (88, 92) is orthogonally disposed with respect to said axis of said third
and fourth flexible linkages (36, 38).
11. The micromechanical gyroscopic transducer of claims 6, 7 or 8,
characterized in that
said slot (86, 90) is trimmed to adjust a beam (94, 98) formed by said slot, said
beam defining a resonant frequency of said first gimbal plate (32) as supported by
said first and second flexible linkages (20, 22).
12. The micromechanical gyroscopic transducer of claims 6, 9 or 10,
characterized in that
said slot (88, 92) is trimmed to adjust a beam (96, 100) formed by said slot, said
beam defining a resonant frequency of said second gimbal plate (34).
13. The micromechanical gyroscopic transducer of claim 1,
characterized in that
at least two opposite ones of said flexible linkages (36, 38) further include a depressed
portion (102, 104) extending in a direction parallel to the axis defined by said opposite
linkages to stiffen said linkages against buckling and bending without corresponding
torsional stiffening.
14. The micromechanical gyroscopic transducer of claim 13,
characterized in that
said depressed portion (102, 104) is formed by plasma etching.
15. The micromechanical gyroscopic transducer of claim 13,
characterized in that
said depressed portion (102, 104) is formed in said flexible linkages (36, 38) by
anisotropic etching.
16. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said first and second flexible linkages (20, 22, 36, 38) join said frame (16) at a
footing region (84) of doped material which region being beyond said first ends of
said first and second flexible linkages to reduce twisting thereof.
17. The micromechanical gyroscopic transducer of claim 16,
characterized in that
said footing region (84) is a P-type material.
18. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said substantially balanced mass (48) comprises a gold plated top portion extending
above said void (14).
19. The micromechanical gyroscopic transducer of claim 18,
characterized in that
said balanced mass (48) includes a polysilicon portion under said gold top portion.
20. The micromechanical gyroscopic transducer of claim 18,
characterized in that
said balanced mass (48) includes a single crystal silicon portion under said gold
top portion.
21. The micromechanical gyroscopic transducer of claim 18,
characterized in
having a titanium tungsten metal layer below said gold.
22. The micromechanical gyroscopic transducer of claim 21,
characterized in
having a gold layer above the titanium tungsten layer.
23. The micromechanical gyroscopic transducer of claim 22,
characterized in that
said titanium tungsten and gold layers are deposited by vacuum deposition.
24. The micromechanical gyroscopic transducer of claim 18,
characterized in that
said gold mass is plated on said second metal by electroplating.
25. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said integral electrodes (50, 52, 54, 56) are formed as a highly doped P-type region
patterned on an N-type silicon sub-surface.
26. The micromechanical gyroscopic transducer of claim 25,
characterized in that
said void (14) is in an N-type layer epitaxially grown over said sub-surface.
27. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said integral electrodes (50, 52, 54, 56) are electrically connected through a doped
region to a metallized contact on said silicon frame (16).
28. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said bridge electrodes (58, 60, 62, 64) are configured above and facing said second
gimbal plate (34).
29. The micromechanical gyroscopic transducer of claim 1,
characterized in that
said region of doped material (111, 112, 114) comprises an isolating wall (114), an
isolating floor (112) and an isolating intermediate area (111) and a driven shield.
30. The micromechanical gyroscopic transducer of claim 29,
characterized in that
said isolating wall (114) and said isolating floor (112) comprise P-type doped semiconductor
material.
31. The micromechanical gyroscopic transducer of claim 29,
characterized in that
said isolating intermediate area (111) is an N-type semiconductor material.
32. The micromechanical gyroscopic transducer of claim 1,
characterized in
further comprising a junction field effect transistor (Q1) fabricated in said semiconductor mass (12).
33. The micromechanical gyroscopic transducer according to one of the preceding claims,
characterized in that
said gimbal plates (32, 34) are thicker than said flexible linkages (20, 22, 36, 38).
1. Mikromechanischer gyroskopischer Wandler mit einer Masse (12) aus Halbleitermaterial,
die eine auf der oberen Fläche nach unten erstreckende Aussparung (14) besitzt, wobei
die Masse aus Silicium einen Siliciumrahmen (16) aufweist;
einem Wandlerelement (18), welches oberhalb der Aussparung (14) aufgehängt ist, wobei
das Wandlerelement (18) aufweist:
erste und zweite flexible Verbindungen (20, 22), welche einteilig mit dem Rahmenmaterial
(16) verbunden sind zum Koppeln des Wandlerelements an den Rahmen (16) an entgegengesetzten
Enden, wobei erste Enden (24, 26) der ersten flexiblen Verbindungen (20, 22) mit dem
Siliciumrahmen (16) verbunden sind;
eine erste Kardanrahmenplatte (32), die einteilig mit dem Rahmenmaterial (16) verbunden
ist und an zweite Enden (28, 30) der ersten und zweiten flexiblen Verbindungen (20,
22) angeschlossen ist, wobei die erste Kardanrahmenplatte (32) zu einer Oszillationsbewegung
um eine durch die ersten und zweiten flexiblen Verbindungen (20, 22) gelegene Achse
fähig ist;
eine zweite Kardanrahmenplatte (34), welche innerhalb der ersten Kardanrahmenplatte
(32) liegt;
dritte und vierte flexible Verbindungen (36, 38), welche einteilig mit dem Rahmenmaterial
(16) verbunden sind und die zweite Kardanrahmenplatte (34) an die erste Kardanrahmenplatte
(32) an entgegengesetzten Enden koppelt, wobei die dritten und vierten flexiblen Verbindungen
(36, 38) erste Enden (40, 42) und zweite Enden (44, 46) besitzen, wobei die ersten
Enden der dritten und vierten flexiblen Verbindungen (36, 38) an die erste Kardanrahmenplatte
(32) angeschlossen sind und die zweiten Enden der dritten und vierten flexiblen Verbindungen
(36, 38) an die zweite Kardanrahmenplatte (34) angeschlossen sind, wobei die zweite
Kardanrahmenplatte (34) zu einer Oszillationsbewegung um eine durch die dritten und
vierten flexiblen Verbindungen (36, 38) gelegte Achse fähig ist;
eine im wesentlichen ausgeglichene Masse (48), welche zentral zu der zweiten Kardanrahmenplatte
(34) angeordnet ist, wobei die im wesentlichen ausgeglichene Masse (48) eine Oberseite
und eine Bodenseite besitzt, die eine dazwischen gelegene Achse festlegen;
erste und zweite Gruppen von Elektroden (50, 52, 54, 56), welche innerhalb der Masse
(12) in einem Bodenbereich der Aussparung (14) angeordnet sind und integral bzw. einteilig
mit dem Rahmenmaterial verbunden sind, wobei die ersten Gruppen von integralen Elektroden
der ersten Kardanrahmenplatte (32) und die zweite Gruppe von integralen Elektroden
der zweiten Kardanrahmenplatte (34) gegenüberliegen;
dadurch gekennzeichnet, daß
eine Vielzahl von Brückenelektroden (58, 60, 62, 64) oberhalb des Wandlerelements
(18) angeordnet ist, wobei jede aus der Vielzahl von Brückenelektroden (58, 60, 62,
64) von dem Rahmen (16) an einer Elektrodenkontaktfläche (106, 108) gelagert ist und
sich über wenigstens eine der ersten (32) und zweiten (34) Kardanrahmenplatten erstreckt,
wobei jede der Brückenelektroden (58, 60, 62, 64) von dem Rahmen an einem Bereich
aus dotiertem Material (111, 112, 114) gelagert ist, welcher zwischen den Brückenelektroden
(58, 60, 62, 64) und dem Massematerial (12) angeordnet ist und mit diesen in elektrischer
Verbindung steht, wobei der Bereich aus dotiertem Material (111, 112, 114) einen dazwischen
gelegenen Bereich (111) aufweist, der durch die umgebenden Bereiche (112, 114) isoliert
ist, wobei der dazwischen gelegene Bereich (111) bei Gebrauch relativ zu dem Massematerial
(12) zur effektiven Isolation der Brückenelektroden (58, 60, 62, 64) von dem Massematerial
(12) vorgespannt ist.
2. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die Masse (12) monokristallines Silicium (15) ist und die Aussparung (14) anisotropisch
darin geätzt ist.
3. Mikromechanischer gyroskopischer Wandler nach Anspruch 2,
dadurch gekennzeichnet, daß
die erste und zweite Kardanrahmenplatte (32, 34) ätzresistente Dotierungssubstanzen
enthalten und durch selektives Ätzen der Masse (12) gebildet sind.
4. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die flexiblen Verbindungen (20, 22, 36, 38) ätzresistente Dotierungssubstanzen enthalten
und durch selektives Ätzen der Masse (12) gebildet sind.
5. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die erste Kardanrahmenplatte (32) eine Einrichtung (94, 96, 98, 100) zum Abbauen von
mechanischer Spannung neben einer oder mehr der flexiblen Verbindungen (20, 22, 36,
38) enthält.
6. Mikromechanischer gyroskopischer Wandler nach Anspruch 5,
dadurch gekennzeichnet, daß
die Einrichtung zum Abbauen von mechanischer Spannung einen Träger (94, 96, 98, 100)
aufweist, welcher durch einen Schlitz (86, 88, 90, 92) gebildet ist.
7. Mikromechanischer gyroskopischer Wandler nach Anspruch 6,
dadurch gekennzeichnet, daß
der Schlitz (86, 90) nahe an den zweiten Enden der ersten und zweiten flexiblen Verbindungen
(20, 22) gelegen ist.
8. Mikromechanischer gyroskopischer Wandler nach Anspruch 6,
dadurch gekennzeichnet, daß
der Schlitz (86, 90) in bezug auf die Achse der ersten und zweiten flexiblen Verbindungen
(20, 22) orthogonal angeordnet ist.
9. Mikromechanischer gyroskopischer Wandler nach Anspruch 6,
dadurch gekennzeichnet, daß
der Schlitz (88, 92) nahe an den ersten Enden der dritten und vierten flexiblen Verbindungen
(36, 38) gelegen ist.
10. Mikromechanischer gyroskopischer Wandler nach Anspruch 6,
dadurch gekennzeichnet, daß
der Schlitz (88, 92) in bezug auf die Achse der dritten und vierten flexiblen Verbindungen
(36, 38) orthogonal angeordnet ist.
11. Mikromechanischer gyroskopischer Wandler nach Anspruch 6, 7 oder 8,
dadurch gekennzeichnet, daß
der Schlitz (86, 90) zur Einstellung eines durch den Schlitz gebildeten Trägers (94,
98) geschnitten bzw. angekantet ist, wobei der Träger eine Resonanzfrequenz der ersten
Kardanrahmenplatte (32) bei Lagerung durch die ersten und zweiten flexiblen Verbindungen
(20, 22) bestimmt.
12. Mikromechanischer gyroskopischer Wandler nach Anspruch 6, 9 oder 10,
dadurch gekennzeichnet, daß
der Schlitz (88, 92) zum Anpassen eines durch den Schlitz gebildeten Trägers (96,
100) geschnitten bzw. abgekantet ist, wobei der Träger eine Resonanzfrequenz der zweiten
Kardanrahmenplatte (34) bestimmt.
13. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
wenigstens zwei der gegenüberliegenden flexiblen Verbindungen (36, 38) ferner einen
abgesenkten Abschnitt (102, 104) enthalten, welcher sich in einer parallel zu der
durch die gegenüberliegenden Verbindungen bestimmten Achse verlaufenden Richtung erstreckt
zur Versteifung der Verbindungen gegen Krümmen und Biegen ohne entsprechende Torsionsversteifung.
14. Mikromechanischer gyroskopischer Wandler nach Anspruch 13,
dadurch gekennzeichnet, daß
der abgesenkte Abschnitt (102, 104) durch Plasmaätzen gebildet ist.
15. Mikromechanischer gyroskopischer Wandler nach Anspruch 13,
dadurch gekennzeichnet, daß
der abgesenkte Abschnitt (102, 104) in die flexiblen Verbindungen (36, 38) durch anisotropisches
Ätzen gebildet ist.
16. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die ersten und zweiten flexiblen Verbindungen (20, 22, 36, 38) sich an den Rahmen
(16) an einem Fußbereich (84) aus dotiertem Material anschließen, wobei der Bereich
jenseits der ersten Enden der ersten und zweiten flexiblen Verbindungen zur Verminderung
von deren Verdrehung gelegen ist.
17. Mikromechanischer gyroskopischer Wandler nach Anspruch 16,
dadurch gekennzeichnet, daß
der Fußbereich (84) ein P-Typ Material ist.
18. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die im wesentlichen ausgeglichene Masse (48) einen goldüberzogenen oberen Abschnitt
aufweist, welcher sich oberhalb der Aussparung (14) erstreckt.
19. Mikromechanischer gyroskopischer Wandler nach Anspruch 18,
dadurch gekennzeichnet, daß
die ausgeglichene Masse (48) einen unter dem Goldoberabschnitt liegenden Polysiliciumabschnitt
enthält.
20. Mikromechanischer gyroskopischer Wandler nach Anspruch 18,
dadurch gekennzeichnet, daß
die ausgeglichene Masse (48) einen Einkristall-Siliciumabschnitt unterhalb des Goldoberabschnittes
enthält.
21. Mikromechanischer gyroskopischer Wandler nach Anspruch 18,
dadurch gekennzeichnet, daß
er unterhalb des Goldes eine Titan-Wolfram-Metallschicht aufweist.
22. Mikromechanischer gyroskopischer Wandler nach Anspruch 21,
dadurch gekennzeichnet, daß
er oberhalb der Titan-Wolfram-Schicht eine Goldschicht aufweist.
23. Mikromechanischer gyroskopischer Wandler nach Anspruch 22,
dadurch gekennzeichnet, daß
die Titan-Wolfram- und die Goldschichten durch Vakuumaufdampfung abgelagert sind.
24. Mikromechanischer gyroskopischer Wandler nach Anspruch 18,
dadurch gekennzeichnet, daß
die Goldmasse auf das zweite Metall durch Galvanisieren überzogen ist.
25. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die integralen Elektroden (50, 52, 54, 56) als ein hochdotierter P-Typ Bereich gebildet
sind, welcher auf einer N-Typ Siliciumunterfläche strukturiert ist.
26. Mikromechanischer gyroskopischer Wandler nach Anspruch 25,
dadurch gekennzeichnet, daß
die Aussparung (14) eine N-Typ Schicht ist, welche epitaxial über der Unterfläche
aufgewachsen ist.
27. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die integralen Elektroden (50, 52, 54, 56) elektrisch durch einen dotierten Bereich
an einen metallisierten Kontakt auf dem Siliciumrahmen (16) angeschlossen sind.
28. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
die Brückenelektroden (58, 60, 62, 64) oberhalb der zweiten Kardanrahmenplatte (34)
angeordnet sind und dieser gegenüberliegen.
29. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
der Bereich aus dotiertem Material (111, 112, 114) eine Isolationswandung (114), einen
Isolationsboden (112) und einen isolierenden, dazwischen gelegenen Bereich (111) sowie
eine angetriebene Schirmung aufweist.
30. Mikromechanischer gyroskopischer Wandler nach Anspruch 29,
dadurch gekennzeichnet, daß
die Isolationswandung (114) und der Isolationsboden (112) P-Typ dotiertes Halbleitermaterial
aufweisen.
31. Mikromechanischer gyroskopischer Wandler nach Anspruch 29,
dadurch gekennzeichnet, daß
der isolierende, dazwischen gelegene Bereich (111) ein N-Typ Halbleitermaterial ist.
32. Mikromechanischer gyroskopischer Wandler nach Anspruch 1,
dadurch gekennzeichnet, daß
er einen Sperrschichtfeldeffekt-Transistor (Q1) aufweist, welcher in der Halbleitermasse (12) hergestellt ist.
33. Mikromechanischer gyroskopischer Wandler nach einem der vorangehenden Ansprüche,
dadurch gekennzeichnet, daß
die Kardanrahmenplatten (32, 34) dicker sind als die flexiblen Verbindungen (20, 22,
36, 38).
1. Transducteur gyroscopique micromécanique comportant : une masse (12) de matériau semiconducteur
possédant un vide (14) sur une surface supérieure s'étendant vers le bas, ladite masse
de silicium comportant un cadre de silicium (16);
un élément transducteur (18) suspendue au-dessus dudit vide (14), ledit élément transducteur
(18) comportant :
des première et seconde liaisons flexibles (20, 22) faisant corps avec ledit matériau
de cadre (16) pour relier ledit élément transducteur audit cadre (16) en des extrémités
opposées, les premières extrémités (24, 26) desdites premières liaisons flexibles
(20, 22) étant reliées audit cadre de silicium (16);
une première plaque suspendue (32) faisant corps avec ledit matériau de cadre (16)
reliée auxdites secondes extrémités (28, 30) desdites première et seconde liaisons
flexibles (20, 22), ladite première plaque suspendue (32) pouvant décrire un mouvement
oscillant autour d'un axe par l'intermédiaire desdites première et seconde liaisons
flexibles (20, 22);
une seconde plaque suspendue (34), intérieure à ladite première plaque suspendue (32);
des troisièmes et quatrième liaisons flexibles (36, 38) faisant corps avec ledit matériau
de cadre (16) reliant ladite seconde plaque suspendue (34) à ladite première plaque
suspendue (32) sur les extrémités opposées, lesdites troisième et quatrième liaisons
flexibles (36, 38) possédant des premières extrémités (40, 42) et des secondes extrémités
(44, 46), lesdites premières extrémités desdites troisième et quatrième liaisons flexibles
(36, 38) étant reliées à ladite première plaque suspendue (32) et lesdites secondes
extrémités desdites troisième et quatrième liaisons flexibles (36, 38) étant reliées
à ladite seconde plaque suspendue (34), ladite seconde plaque suspendue (34) pouvant
décrire un mouvement oscillant autour d'un axe par l'intermédiaire desdites troisième
et quatrième liaisons flexibles (36, 38);
une masse sensiblement équilibrée (48) au centre de ladite seconde plaque suspendue
(34), ladite masse sensiblement équilibrée (48) possédant un côté supérieur et un
côté inférieur définissant un axe entre eux;
des premier et second ensembles d'électrodes (50, 52, 54, 56) configurés à l'intérieur
de ladite masse (12) dans une région inférieure dudit vide (14) et faisant corps avec
ledit matériau de cadre, ledit premier ensemble d'électrodes faisant corps étant tourné
vers ladite première plaque suspendue (32) et ledit second ensemble électrodes faisant
corps étant tourné vers ladite seconde plaque suspendue (34);
caractérisé en ce que
une pluralité d'électrodes en pont (58, 60, 62, 64) sont configurées au-dessus dudit
élément transducteur (18), chacune de ladite pluralité d'électrodes en pont (58, 60,
62, 64), étant supportée par ledit cadre (16) sur une partie surélevée d'électrode
(106, 108) et s'étendant au-dessus d'au moins l'une desdites première (32) et seconde
(34) plaques suspendues,
chacune desdites électrodes en pont (58, 60, 62, 64) est supportée depuis ledit cadre
sur une région de matériau dopé (111, 112, 114) disposée entre et en communication
électrique avec lesdites électrodes en pont (58, 60, 62, 64), et ledit matériau de
masse (12), dans lequel ladite région de matériau dopé (112, 114) comporte une région
intermédiaire (111) isolée par des régions environnantes (112, 114), ladite région
intermédiaire (111), en utilisation, étant polarisée par rapport audit matériau de
masse, de manière à isoler efficacement lesdites électrodes en pont (58, 60, 62, 64)
dudit matériau de masse (12).
2. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que ladite masse (12) est en silicium monocristallin (15) et ledit vide (14) est
gravé de façon anisotrope à l'intérieur.
3. Transducteur gyroscopique micromécanique selon la revendication 2, caractérisé en
ce que lesdites première et seconde plaques suspendues (32, 34) comprennent des dopants
résistant à la gravure et sont formées par gravure sélective de ladite masse (12).
4. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que lesdites liaisons flexibles (20, 22, 36, 38) comprennent des dopants résistant
à la gravure et sont formées par gravure sélective de ladite masse (12).
5. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que ladite première plaque suspendue (32) comprend les moyens (94, 96, 98, 100)
pour atténuer une contrainte adjacente à une ou à plusieurs desdites liaisons flexibles
(20, 22, 36, 38).
6. Transducteur gyroscopique micromécanique selon la revendication 5, caractérisé en
ce que lesdits moyens de relâchement de contrainte comportent une poutre (94, 96,
98, 100) créée par une fente (86, 88, 90, 92).
7. Transducteur gyroscopique micromécanique selon la revendication 6, caractérisé en
ce que ladite fente (86, 90) se trouve à proximité desdites secondes extrémités desdites
première et seconde liaisons flexibles (20, 22).
8. Transducteur gyroscopique micromécanique selon la revendication 6, caractérisé en
ce que ladite fente (86, 90) est disposée orthogonalement par rapport audit axe desdites
première et seconde liaisons flexibles (20, 22).
9. Transducteur gyroscopique micromécanique selon la revendication 6, caractérisé en
ce que ladite fente (88, 92) est à proximité desdites premières extrémités desdites
troisième et quatrième liaisons flexibles (36, 38).
10. Transducteur gyroscopique micromécanique selon la revendication 6, caractérisé en
ce que ladite fente (88, 92) est disposée orthogonalement par rapport audit axe desdites
troisième et quatrième liaisons flexibles (36, 38).
11. Transducteur gyroscopique micromécanique selon les revendications 6, 7 ou 8, caractérisé
en ce que ladite fente (86, 90) est taillée pour ajuster une poutre (94, 98) formée
par ladite fente, ladite poutre définissant une fréquence de résonance de ladite première
plaque suspendue (32) telle que supportée par lesdites première et seconde liaisons
flexibles (20, 22).
12. Transducteur gyroscopique micromécanique selon les revendications 6, 9 ou 10, caractérisé
en ce que ladite fente (88, 90) est taillée pour ajuster une poutre (96, 100) formée
par ladite fente, ladite poutre définissant une fréquence de résonance de ladite seconde
plaque suspendue (34).
13. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce qu'au moins deux liaisons opposées desdites liaisons flexibles (36, 38) comprennent
en outre une partie évidée (102, 104) s'étendant dans une direction parallèle à l'axe
défini par lesdites liaisons opposées afin de renforcer lesdites liaisons contre un
flambage et une flexion sans renfort correspondant en torsion.
14. Transducteur gyroscopique micromécanique selon la revendication 13, caractérisé en
ce que ladite partie évidée (102, 104) est formée par gravure par plasma.
15. Transducteur gyroscopique micromécanique selon la revendication 13, caractérisé en
ce que ladite partie évidée (102, 104) est formée dans lesdites liaisons flexibles
(36, 38) par gravure anisotrope.
16. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que lesdites première et seconde liaisons flexibles (20, 22, 36, 38) réunissent
ledit cadre (16) en une région d'embase (84) de matériau dopé, ladite région se trouvant
au-delà desdites premières extrémités desdites première et seconde liaisons flexibles
pour réduire la torsion de celles-ci.
17. Transducteur gyroscopique micromécanique selon la revendication 16, caractérisé en
ce que ladite région d'embase (84) est un matériau de type P.
18. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que ladite masse sensiblement équilibrée (48) comporte une partie supérieure revêtue
d'or s'étendant au-dessus dudit vide (14).
19. Transducteur gyroscopique micromécanique selon la revendication 18, caractérisé en
ce que ladite masse équilibrée (48) comprend une partie en silicium polycristallin
au-dessous de ladite partie supérieure dorée.
20. Transducteur gyroscopique micromécanique selon la revendication 18, caractérisé en
ce que ladite masse équilibrée (48) comprend une partie en silicium monocristallin
au-dessous de ladite partie supérieure dorée.
21. Transducteur gyroscopique micromécanique selon la revendication 18, caractérisé en
ce qu'il possède une couche de métal en titane tungstène au-dessous dudit or.
22. Transducteur gyroscopique micromécanique selon la revendication 21, caractérisé en
ce qu'il possède une couche d'or au-dessus de la couche de titane tungstène.
23. Transducteur gyroscopique micromécanique selon la revendication 22, caractérisé en
ce que lesdites couches de titane, de tungstène et d'or sont déposées sous vide.
24. Transducteur gyroscopique micromécanique selon la revendication 18, caractérisé en
ce que ladite masse d'or est déposée électrolytiquement sur ledit second métal.
25. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que lesdites électrodes faisant corps (50, 52, 54, 56) sont réalisées sous la forme
d'une région de type P fortement dopée configurée sur un substrat de silicium de type
N.
26. Transducteur gyroscopique micromécanique selon la revendication 25, caractérisé en
ce que ledit vide (14) est une couche épitaxiale de type N au-dessus dudit substrat.
27. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que lesdites électrodes faisant corps (50, 52, 54, 56) sont reliées électriquement
par l'intermédiaire d'une région dopée à un contact métallisé sur ledit cadre de silicium
(16).
28. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que lesdites électrodes en pont (58, 60, 62, 64) sont configurées au-dessus et
tournées vers ladite seconde plaque suspendue (34).
29. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce que ladite région de matériau dopé (111, 112, 114) comporte une paroi isolante
(114), un fond isolant (112) et une région intermédiaire isolante (111) et un blindage
commandé.
30. Transducteur gyroscopique micromécanique selon la revendication 29, caractérisé en
ce que ladite paroi isolante (114) et ledit fond isolant (112) comportent un matériau
dopé de type P.
31. Transducteur gyroscopique micromécanique selon la revendication 29, caractérisé en
ce que ladite région intermédiaire isolante (111) est un matériau semiconducteur de
type N.
32. Transducteur gyroscopique micromécanique selon la revendication 1, caractérisé en
ce qu'il comporte en outre un transducteur à effet de champ à jonction (Q1) réalisé dans ladite masse semiconductrice (12).
33. Transducteur gyroscopique micromécanique selon l'une des revendications précédentes,
caractérisé en ce que lesdites plaques suspendues (32, 34) sont plus épaisses que
lesdites liaisons flexibles (20, 22, 36, 38).